首页> 外文期刊>IEICE Transactions on Electronics >Efficient Computation of MoM Matrix Elements in Analysis of General Microstrip Structure
【24h】

Efficient Computation of MoM Matrix Elements in Analysis of General Microstrip Structure

机译:通用微带结构分析中MoM矩阵元素的有效计算

获取原文
获取原文并翻译 | 示例
       

摘要

An efficient method for calculating impedance matrix elements is proposed for analysis of micro-strip structures with an arbitrary substrate thickness. Closed-form Green's functions are derived by applying the GPOF method to the remaining function after the extraction of the contributions of the surface wave pole, source dipole itself, and quasi-static (i.e. real images) from a spectral domain Green's function. When closed-form Green's functions are used in conjunction with rooftop-pulse subsectional basis functions and the razor testing function in an MoM with an MPIE formulation, the integrals appearing in the calculation procedure of the diagonal matrix elements are of two types. The first is ∫ ∫ x_0~n [e~(-jk_0 (x_0~2+y_0~2+a~2)~(1/2)) /(x_0~2 + y_0~2+a~2)~(1/2)] dx_0dy_0 (where n = 0, 1) for the contribution of both the source dipole itself or real images where a = 0 and complex images where a = complex constant, while the other is ∫ ∫ x_0~nH_0~((2)) (k_(ρp) (x_0~2 + y_0~2)~(1/2))dx_0dy_0 for the contribution of the surface wave pole where k_(ρp) is a real pole due to the surface wave. Adopting a polar coordinate for the integral for both cases of n = 0 and n = 1 and performing analytical integrations for n = 1 with respect to the variable x_0 for both types not only removes the singularities but also drastically reduces the evaluation time for the numerical integration. In addition, the above numerical efficiency is also retained for the off-diagonal elements. To validate the proposed method, several numerical examples are presented.
机译:提出了一种计算阻抗矩阵元素的有效方法,以分析具有任意衬底厚度的微带结构。封闭形式的格林函数是通过从频谱域格林函数中提取出表面波极,源偶极子本身和准静态(即实像)的贡献后,将GPOF方法应用于其余函数而得出的。在具有MPIE公式的MoM中,当闭合形式的Green函数与屋顶脉冲分段基本函数和剃刀测试函数结合使用时,对角矩阵元素的计算过程中出现的积分有两种。第一个是∫∫x_0〜n [e〜(-jk_0(x_0〜2 + y_0〜2 + a〜2)〜(1/2))/(x_0〜2 + y_0〜2 + a〜2)〜( 1/2)] dx_0dy_0(其中n = 0,1)表示源偶极子本身或a = 0的实像和a =复数常数的复数图像,而另一个是∫∫x_0〜nH_0〜( (2))(k_(ρp)(x_0〜2 + y_0〜2)〜(1/2))dx_0dy_0对于表面波极的贡献,其中k_(ρp)是由于表面波引起的实极。对n = 0和n = 1的情况均采用极坐标作为积分,并对两种类型的变量x_0进行n = 1的解析积分,不仅消除了奇点,而且大大减少了数值求值时间积分。另外,对于非对角线元素也保持上述数值效率。为了验证所提出的方法,给出了几个数值示例。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号